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Physical review. B, Solid state

Observability of Josephson pair-quasiparticle interference in superconducting interferometers

Paul K. Hansma

Published Sep 1, 1975• 18 citations
Publisher

Abstract

Pair-quasiparticle interference current has a measurable effect on the tuning characteristics of a superconducting interferometer operating in the nonhysteretic regime: $\ensuremath{\epsilon}\ensuremath{\equiv}(\frac{2\ensuremath{\pi}}{{\ensuremath{\Phi}}_{0}}){L}_{R}{I}_{c}<1$ where ${\ensuremath{\Phi}}_{0}=\frac{h}{2e}$, ${L}_{R}$ is the inductance of the interferometer ring, and ${I}_{c}$ is the critical current of the interferometer's weak link. In the limit $\ensuremath{\epsilon}\ensuremath{\ll}1$ the interferometer will have a zero crossing in its magnetic flux sensitivity versus frequency characteristic that is above, on, or below resonance depending whether the coefficient of the interference current term is positive, zero, or negative, respectively. For larger $\ensuremath{\epsilon}$, screening currents will also shift the zero crossing. Results for the magnitude of this additional shift are presented and discussed.

DOI
10.1103/physrevb.12.1707

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Pair-quasiparticle interference current has a measurable effect on the tuning characteristics of a superconducting interferometer operating in the nonhysteretic regime: \ensuremathϵ\ensuremath≡(2\ensuremathπ\ensuremathΦ0)LRIc<1\ensuremath{\epsilon}\ensuremath{\equiv}(\frac{2\ensuremath{\pi}}{{\ensuremath{\Phi}}_{0}}){L}_{R}{I}_{c}<1\ensuremathϵ\ensuremath≡(\ensuremathΦ0​2\ensuremathπ​)LR​Ic​<1 where \ensuremathΦ0=h2e{\ensuremath{\Phi}}_{0}=\frac{h}{2e}\ensuremathΦ0​=2eh​, LR{L}_{R}LR​ is the inductance of the interferometer ring, and Ic{I}_{c}Ic​ is the critical current of the interferometer's weak link. In the limit \ensuremathϵ\ensuremath≪1\ensuremath{\epsilon}\ensuremath{\ll}1\ensuremathϵ\ensuremath≪1 the interferometer will have a zero crossing in its magnetic flux sensitivity versus frequency characteristic that is above, on, or below resonance depending whether the coefficient of the interference current term is positive, zero, or negative, respectively. For larger \ensuremathϵ\ensuremath{\epsilon}\ensuremathϵ, screening currents will also shift the zero crossing. Results for the magnitude of this additional shift are presented and discussed.
The LC\mathrm{LC}LC (inductance-capacitance) resonance phenomenon in the dc SQUID (superconducting quantum interference device) creates a current peak in the $I\ensuremath{-}V$ characteristics at a voltage determined by the resonance frequency. These $I\ensuremath{-}V$ characteristics have been analyzed with the resistively shunted Josephson-junction model in the low-damping and small-oscillation regime. The resonance $I\ensuremath{-}V$ characteristics contain sufficient information to determine all circuit parameters for the dc SQUID's. Specifically, we can apply this analysis to symmetric, tunnel-junction dc SQUID's to deduce the pair-quasiparticle interference conductance ($cos\ensuremath{\theta}$ term).
Nanoscale superconducting quantum interference devices (nano-SQUIDS) where the weak links are made from nanobridges, i.e., nanobridge SQUIDs (NBSs), are one of the most sensitive magnetometers for nanoscale magnetometry. Because of very strong nonlinearity in the nanobridge-electrode joints, the applied magnetic flux (${\mathrm{\ensuremath{\Phi}}}_{a}$)--critical current (Ic{I}_{c}Ic​) characteristics of NBSs differ very significantly from conventional tunnel-junction SQUIDs, especially when the nanobridges are long and/or the screening parameter is large. However, in most of the theoretical descriptions, NBSs have been treated as the conventional tunnel-junction SQUIDs, which are based on the dc Josephson effect. Here, I present a model demonstrating that for long nanobridges and/or large screening parameters the ${I}_{c}({\mathrm{\ensuremath{\Phi}}}_{a})$ of a NBS can be explained by merely considering the fluxoid quantization in the NBS loop and the energy of the NBS; it is not necessary to take the Josephson effect into consideration. I also demonstrate that using the model, one can derive useful expressions such as the modulation depth and transfer function. I discuss the role of the kinetic inductance fraction ($\ensuremath{\kappa}$) in determining ${I}_{c}({\mathrm{\ensuremath{\Phi}}}_{a})$. I compare the predictions of the present model with the experimental data already published by several groups.
The operation of a constant-current quantum interferometer with two Josephson junctions is studied in a system for measuring small changes in a magnetic field with low-frequency modulation of the magnetic flux. Idealized theoretical signal characteristics are found together with their dependence on the operating mode and parameters of a SQUID. These characteristics are used in Pt. II (ref. 12) to determine the minimal detectable change in the magnetic flux, which characterizes the maximal sensitivity of a SQUID.
A study is made of the effects of quantum interference in weakly coupled superconducting systems in an external magnetic field, allowance being made for fluctuations. The circulating supercurrent is found as a function of the applied magnetic field for a weakly coupled ring when the coupling is comparable in magnitude with the thermal energy. The current--voltage characteristic for a superconducting quantum interferometer is found and it is shown that the amplitude of the steps formed in the current--voltage characteristic under the influence of external irradiation is an oscillating function of the flux of the applied magnetic field with a period equal to the flux quantum. (AIP)
A simple theory of the superconducting single-junction interferometer (ac Squid) becomes possible if the critical current of the single junction is small relative to Φ0/LR, where Φ0=h/2e is one flux quantum and LR is the inductance of the interferometer loop. This theory predicts a magnetic flux sensitivity which has the same dependence on interferometer parameters as the existing theories for higher critical currents. In contrast to those theories, however, the present theory predicts that the maximum flux sensitivity will be achieved off resonance. Theoretical predictions for comparison with experiment are displayed as a function of the normalized difference between the operating frequency ω and the resonant frequency ω0.